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A NNALES DE L ’I. H. P., SECTION A

P. G RZEGORCZYK

F. P RZYTYCKI W. S ZLENK

On iterations of Misiurewicz’s rational maps on the Riemann sphere

Annales de l’I. H. P., section A, tome 53, n

o

4 (1990), p. 431-444

<http://www.numdam.org/item?id=AIHPA_1990__53_4_431_0>

© Gauthier-Villars, 1990, tous droits réservés.

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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

(2)

431

On iterations of Misiurewicz’s rational maps

on

the Riemann sphere

P. GRZEGORCZYK, F. PRZYTYCKI and W. SZLENK Polish Academy of Sciences, Institute of Mathematics, ul.

Sniadeckich 8, 00-950 Warszawa, Poland Warsaw University, Department of Mathematics,

PKiN 9 p., 00-901 Warszawa, Poland

Vol. 53, 4, 1990, Physique théorique

ABSTRACT. - This paper concerns

ergodic properties

of rational maps of the Riemann

sphere,

of

subexpanding

behaviour. In

particular

we prove the existence of an

absolutely

continuous invariant measure,

study

its

density

and prove the metric exactness..

This is not a

strictly

research paper. Its aim is to present useful facts

belonging

to the folklore but

partially

not

explicitly published

up to now.

INTRODUCTION

Let f

be a rational map of a Riemann

sphere f,

let J denote its Julia set, y denote the

normalised,

standard Riemann measure on

ê

Derivatives in the paper are considered

usually

with respect to the Riemann metric.

Annales de l’Institut Henri Poincaré - Physique théorique - 0246-0211 1

Vol. 53/90/04/43 1 /14/$3.40/ © Gauthier-Villars

(3)

In this text we

verify

under suitable

assumptions

two

properties:

The property

(ii)

is called metric exactness. Satisfaction of the both

properties

without any additional

assumptions

is a famous open

problem;

we do not make any progress in

solving

it.

Consider also the property

In section 2 we prove

(i)

and

(ii’)

under the

assumption

that all critical

points

in J are

eventually periodic.

In section 3 we consider the case where Crit J

== 0

and moreover

f

is

expanding

on J n the set of

neutral rational

periodic points } (i. e.

there exists k &#x3E; 0 such that for every

z ~ ( f k)’ (z) ~ &#x3E; 1 ).

We call

such f

Misiurewicz’s map

by

the

analogy

with

maps considered in

[M].

In

paragraph

4 in the case we prove the existence of an invariant measure

equivalent

to ~

[this

allows to pass from

(ii’)

to

(ii)]

and prove that outside the set it has

real-analytic

subharmonic

density.

Everything

in this paper is the so called folklore for

specialists,

but

partially

not

explicitly published.

So we decided that this material is

worthy

of

being

written down. Lots of facts from this paper

rely

on

Koebe’s distortion

theorem,

see

[H],

Th. 17.4.6. One version is that for every t 1 and C &#x3E; 0 there exists

C (t) &#x3E; 0

such that for every

holomorphic

univalent

function f : []) --t ê

on the unit

disc,

such that diam

(~B~f ([])))

&#x3E; C

Contrary

to a

recently popular

custom no involvement of a

hyperbolic

metric is necessary. Our text is

elementary.

Let us call the attention of the reader to

significant Mary

Rees’ paper

[R].

Our considerations consti- tute

only

a

starting point

to her

infinitely

more delicate

study.

A part of

our paper

overlaps

also with M.

Lyubich

paper

[L].

This text grew from discussions at the Cornell conference on iterations in

August 1987,

a talk of the second author at the Warsaw

dynamics

seminar and an

unpublished preprint by

the third author.

Remark on the notation. - The letter C will be used to denote various

positive

constants either universal or

dependent only

on

f,

which may

differ from one formula to another even within a

single

stream of estimates.

D will denote the end of a

proof, .

will denote the end of a statement of a

theorem, lemma,

etc.

(4)

1.

BASIC LEMMAS

LEMMA 1. - Let V be an open disc

in f

such that V n

J ~ ~

and V is

disjoint

with a

periodic

orbit

Q

of

period

at least 3.

Suppose

we have a

sequence of backward branches of iterates

of f-1

on

V, namely

holo-

morphic,

univalent functions gn =

f§"’

~n~

Iv,

where m

(n)

- 00 as n -~ 00.

Then the derivatives

g;,

converge to 0

uniformly

on every compact set in V..

Proof -

If the lemma were false then there would exist a

subsequence

gni and

points zi

in a compact subset of V such

that ] &#x3E;

E for a

positive

constant E.

As gni

is a normal

family (the

values omit the set

Q),

there exists a

holomorphic

function G which is the limit of

subsequence

of

(gn)’

for

simplification

denote it also

by (gn)’

and G is non-constant.

Then

by

the invariance and compactness of the Julia set the

point G (p) =

lim

belongs

to

J, provided pEV

n J. One of the

equivalent

definitions of J says that for every

point

in J and its

neighbourhood

A no

subsequence of fn IA

is normal. We conclude

by

Montel’s theorem that for

an

arbitrary

open set V’ such that

V’ 3 G(p)

and cl V’ c

G (V),

for an

arbitrary io

the set U

f m (V’), covers ~

except at most 2

points.

On

the other hand for

every i large enough

gni

(V) ::J

V’ so

f m (V’)

C

V,

a contradiction. D

COROLLARY 1. -

If U is

a

neighbourhood ofcl(Crit+),

then on the

derivatives converge

uniformly

to 0

( for

all backward branches

LEMMA 2. - Let

p E J be a periodic point. Suppose

there exists a

neigh-

bourhood V

of

p such that

(VB~ p })

n Crit + =

0.

Then p is a source..

Proof -

If we

supposed

i. e. we would deduce that p is a source

immediately

from

Corollary

1. Consider the

general

case. Let A be an open

topological

disc

containing precisely

one

point

qA from

O (p),

the

periodic

orbit

of p,

and such that n Crit + =

0.

Consider B a component of the set

1-1 (A) intersecting

O

(p).

Because

flo (p)

is

1- to - l,

B contains

precisely

one

point

qB

belonging

to O

(p).

We have

f (qB)

= qA. The map

f (BB f - ~

is a

covering

map to the annulus So the fundamental group of

(qA)

is a

subgroup

of

Z,

hence

1 (qA)

is an

annulus,

hence the n B consists of one

point

qB

only.

As

qB ~ Crit [otherwise

would be a

sink,

so

p ~ J], f

is a

covering

map from B to the

topological

disc A. So is invertible. We have a

holomorphic

univalent branch

f v 1 :

A - B. Observe that

similarly

Vol. 53, n° 4-1990.

(5)

to A also B has the property n Crit + =

ø.

Indeed if

Z

Efn (Crit)

n

B.,

n &#x3E;

0, then f (Z) (Crit)

fl A so the

only possibility

is

hence a contradiction.

Now we can suppose that V is an open

topological

disc

containing precisely

one

point

from O

(p).

Define

by

induction branches gn = on

V.

Namely having

defined gn we set A = gn

(V)

and define gn + 1 = 1 where

1 :

A ~ B is a map considered above. Now Lemma 2 follows from the Lemma I. 0

COROLLARY 2. - For every neutral

periodic point

p

(i.

e. such that

I ( f n)’ (p) I

=

1,

where n is a

period of p),

there exist a critical

point

c and a

sequence

of integers

ni -~ 00 such that

(c)

--~ p and

fni (c) ~ p..

LEMMA 3. -

Suppose

we have a measurable set E c J and E &#x3E;

0,

such

that

for

a. e. z ~ E there exist a sequence

of positive integers (ni}, points

and branches

of (holomorphic, univalent) defined

on the

respective

discs B

(zi, E)

which map zi to z. Then either ~,

(E)=

0 or there

exists NO such that

( for

one

of

the above

sequences

(ni)}.

.

Proof - Suppose y (E)

&#x3E; 0. Then there exists a

point

of

density

z E

E,

for which the

assumptions

of the lemma are

applicable.

Take a finite

family

of open discs

Dl,

...,

Dm,

of radius

E/4, intersecting J,

such that

m

U

Dj:::::&#x3E;

J. For every i there exists for which It is

j= 1

known

(topological exactness)

that there exist a

neighbourhood %

of J

and an

integer

N &#x3E; 0 such that for

every j

we

have f’~ (D j) :::::&#x3E;

~.

Now

by

Lemma

1,

definition of the

density point

and Koebe’s distortion theorem we have Jl

(, f ’

’~i

(Dj

fi

( f

nt

c~.&#x3E;~

...-+ 1 a Hence

again by

Koebe’s theorem Y

(Dj

(i)

~ fni(E))/ (Dj(i))

-

1,

hence

Jl

(4Y)

- 1. This

implies

in

particular

that J cannot be

nowhere

dense,

so We obtain 1. 0

DEFINITION. - Let us call the set

J""{

dist

( f n (z), (ù) -+ 0 ~

the

transverse limit set and denote it

by

Observe

thatf-1 (~1) = c~l. 1~

LEMMA 4. -

Either ~.

= 0 or ~.

(ro-1-)

=1. In the latter case

for

every measurable set E c with }.l

(E)

&#x3E; 0 we have lim sup

(fn (E))

= 1..

n -~ 00

~’roof. -

Let E c Then there exist E’ c E with and a number 03B4&#x3E;0 such that for every there exists a sequence ni -+ 00 such that dist

(z), ro)

&#x3E; ð. Let N be such an

integer

c

B(CO,ð/2).

So

Crit+)~2-N ö/2,

where 2

is the

Lipschitz

constant

for f

Fix ~ =

-N 03B4/2

and

apply

Lemma 3. 0

(6)

2. THE CASE WHERE ALL CRITICAL POINTS IN J ARE EVENTUALLY PERIODIC

THEOREM 1. -

Suppose

that every

point

c E Crit fl J is

eventually periodic,

i. e. there exist n

(c) ~

0 such

that fn

(c)

(c)

is

periodic.

Then

(a)

every

periodic point

in J which is not neutral rational

(i.

e.

if ( f n)’ (x)

is not a root

of unity,

where n is a a

period)

is a source.

(b)

the

properties (i)

and

(ii’) from

the introduction hold..

Proof -

For every

periodic point p

in

J,

not neutral

rational,

the

assumptions

of Lemma 2 are satisfied. Indeed we may bother

only

about

critical

points

not in L If

eft

J and for a sequence

(.n;),

dist

(fni (c), J)

- 0

then

(f"i (c))

converges to neutral rational

periodic point (by

the classifica- tion of components of

CBJ,

the

theory

of

Julia,

Fatou and

Sullivan).

This proves the assertion

(a).

To prove

(b)

observe that if a

periodic point p

E o is a source then for

zeJ,

for n

large enough.

The

same is true if p is neutral rational. Indeed

(P)

- 0 and

f" (z) ~, f ’n (p)

for every n

imply

that for n

sufficiently large f (z) belongs

to one of the

~petals" (see [DH], Expose IX).

So z is in the

domain of

normality

of iteration

of f,

not in

J,

a contradiction.

(We

owe

the last argument to M.

Lyubich.)

So ~1=

J""-A

where A = U

(ill)

is

countable,

hence of measure 0. The theorem follows now from Lemma 4. D

PROPOSITION 1. -

If all critical points in

are

eventually periodic,

then

there are no neutral

periodic points. If

all critical

points

are

eventually periodic

but not

periodic,

then J =

(C

and all

periodic points

are sources..

Proof -

If all critical

points

are

eventually periodic

then

by Corollary

2

there are no neutral

points

in J. The center of a

Siegel

disc S is also

excluded because as C o and oS is

uncountable,

whereas co is finite. If

additionally

no critical

point

is

periodic, if p

were a sink we would

construct a normal

family

of branches

gn = fn

with p

fixed,

as in the

proof

of the Lemma 2. This

contradicts ~(~))~!/"(~)! 1- I -+ 00.

follows from the Fatou-Julia

theory (lack

of critical

points

to serve

periodic

components of

CBJ)

and Sullivan’s: no

wandering

domains. 0

3. THE CASE WHERE CRITICAL POINTS ARE NOT RECURRENT Let us start with a

general

lemma.

LEMMA 5. - For every real and an

integdr

there exists ~ &#x3E; 0 such that

for

every n and

trajectory

Vol. 53., 4-1990.

(7)

Proof. -

We can suppose that X is

arbitrarity large

and

k =1,

if not,

take an iterate instead

off

and we can compose the branches. 0

THEOREM 2. -

Suppose

that on the set where is

the set

of

all

periodic

neutral rational

points, f

is

expanding,

i. e. there exist

~, &#x3E; 1 and k such that on L we have

I (, f ’k)’ ~ &#x3E;

~,. Then the

properties (i)

and

(ii’) from

introduction are

satisfied..

Proof. -

As in section 2 due to Lemma 4 it is sufficient to prove that J.1 = O. But is the union of the set U

f-n (N ~)

countable

n&#x3E;0 so of measure

0,

and of the set

Write

apply

the Lemma 3 and obtain p

(L03BB)

= O.

So (L’)

= O. D

Remark 1. - In view of Lemma

2,

our Theorem 2 is more

general

than

Theorem 1. One would like to prove the

expanding property

on instead of

assuming it,

but we are not able to do it. This is true for maps of the interval with

negative

Schwarzian derivative

provided

and there are no sinks and neutral

points,

see

[M].

The

reason is that for every E &#x3E; 0 there exist

k&#x3E;0,

such that if

dist ({x,

... ,

J’ M }, Crit) &#x3E;_

s

then (/’ I &#x3E;

1.

Here however the latter assertion is false even in absence of neutral

points

in J. A

counterexample

is

provided by

Michel Herman’s

example

of a

Siegel

disc S not

containing

critical

points

in the

boundary,

see

[D].

(8)

In this

example

is not

expanding

because

where p is the neutral

point

in S and Q is the harmonic measure on as viewed from p. From this

example by

Shishikura’s surgery a counterexam-

ple

with Herman

ring

can be derived.

Another

examples

are

provided by

the maps of the form

/(z)==~z201420142014 2014201420142014,

, with r real close to 0 and see

1- rz z - yr

[Her].

Such a map is of

degree 3,

1=1 is a

diffeomorphism

and for a

suitable

Let us call a closed invariant set in J

disjoint

with

Crit,

on which

j (fk)’

&#x3E; 1 fails for

every k,

a neutral set. The

question

arises what neutral sets are

possible?

Maybe

Crit r) J =

0 implies that/~~% ~ expanding?

This

question

is related to the

question

whether a

periodic

neutral irrational

point

can

attract a critical

point

whose

trajectory

never hits it and to the similar

question

about the

boundary

of a

Siegel disc,

told us

by

M. Herman.

If in the case Crit n 0) U J =

0

a nonempty neutral set different from N f!1I exists the

question

is whether

always u({~-eJ:/"(~)~L}=0

or not?

Remark

finally

that for every A c J such that B

(Crit, E) = 0

for every

n = 0, 1,

..., if for every x E A

then

~, (A) = 0,

see

[L]. (The proof

is similar to that of Lemma 5 and Theorem

2, only

backward iteration should be

replaced by

the forward

one.)

So Theorem 2 holds if the

"expanding" assumption

is

replaced by

the

formally

weaker one: such that

x(/~))&#x3E;0.

We do not

know however of any

example exhibiting

the difference between these

assumptions..

4. ABSOLUTELY CONTINUOUS INVARIANT MEASURE

THEOREM 3. - Under the

assumptions of

Theorem 1 or

2, i. f ’

~,

(J) ~ 0 (i.

e. J =

C),

there exists an invariant measure 11

equivalent

to Jl on

t..

Proof (relying

on the ideas from

[K-S], [M]

and

[S]).

Vol. 53, n° 4-1990.

(9)

1"’

From the sequence of measures y

= - ~ /~ (~~

we choose a

weakly -

*

~ j=c

convergent

subsequence v~i

and consider the limit measure ~ .

For every every small

positive by

Koebe’s distortion theorem

applied

to the

branches f-nv

on the disc

for

every A

c B

(z, 8/2)

we have

where C is a constant

depending only on f.

This follows

precisely

from

cf (*)

from the introduction.

For A = B

(z, t/2)

the

inequality ( 1 ) (the

left hand

side)

~summed up over

all branches

gives

the estimate

independent

of n.

Now for .every n we sum up the

right

hand side

inequality of (1)

over

all branches and deduce from the

resulting

estimate for

from

(2)

and from the definition of r; that r; is

absolutely

continuous with respect to

(write

on

Moreover

We want to know

that ~ ~

on

cl (Crit + )

as well. We have

(cf

the

proof

of Theorem

2).

So we need to prove 11

(cl (Crit + )) = 0

or

equivalenty

11

«(0)=0.

This will be done in Lemma 6.

Meanwhile observe

implies

also the

equivalence

of

11 and u.

Indeed,

take a disc

Bo = B (zo, Eo)

such that 11

(Bo) &#x3E; 0

and

Then

by ( 1 )

the function

I log d~/d I

is bounded

on

Bo,

so 11 and p are

equivalent

on

Bo.

By

and the

property 11 (.~’(A) &#x3E; ~ (A)

for every

A,

the

n z o

equivalence of 11

and Jl holds for every z e

Bc1 {Crit + )

on a disc B

(z,

E

(z))

hence on all of

C.

0

LEMMA 6. -

~((D)=0. N

Proof - By

Lemma 5 and the

expanding property of f on 03C9

the

following

is true:

(4)

there exist

Co, 8,

and À I such that for every n &#x3E; 0 and

y={~...,/"(Jc)}c:B(o,s)

there exists a univalent branch on B

~.~’’~ (x), õ),

to x,

having

distortion on B

(, f’~ (x), õ)

less than

2 and such that

(10)

As critical

points

are attracted to co, there exists N&#x3E;0 such that U

/" (Crit)

c B

(m, s/3).

This

implies

that for every xe

ê

if dist

(x, eo)

~

E/2,

then

dist (x,

U

/"(Crit))~~/6.

Then

n~N

(2

is the

Lipschitz

constant

for f).

Take

b2

8 such that for every disc D

in f

of

radius 2 Co 8~:

(6)

every component

of j- (D)

has diameter less than

8/2

and

(7)

every component

of (D)

has diameter less

than 51 /2.

(Clearly

it suffices to take

ð2 ~

Const

õ1N,

where d is

degree of f. )

Now

take an

arbitrary

disc with

Since (03C9) = 0

there exists a set A c B

(z, ~~/2) containing

B

(z, b2/3j

n ill with Jl

(A) arbitrarily

small and

11

(Fr A)

= 0

hence 11 (A)

= lim

v,~~ (A).

Let us Consider the set g- of all components of Divide ff into n families of sets as follows: for every

k = 0, 1 ,

... , ~ let is the maximal

integer

such that for

every

nf- ~’~({z})

U

B(~s)~0}.

Consider first k = n. Then for every

We used the fact

(4), namely

that

~~ (T)

is 1- to - I and the

respective

branch

~’v ~‘ :

B

(z, ð2)

- T has the distortion bounded

by

2.

Fix now k n and divide

ff k

into two families

For every every reg we have

again

the

inequality (8), only

4 may

change

to another constant.

Consider now

sing’ Write

M = min (N, n - k).

Observe that

where D is

reciprocal

to the maximal

degree

at critical

points.

We leave the first

inequality

as an exercise to the

reader;

the constant

C

depends

on M

(which

is bounded

by N),

so it

depends only

on

f

The

second

inequality similarly

to

(8)

follows from the bounded distortion property

[see (4)].

If M = n - k we obtain from

(9)

Vol. 53, n° 4-1990.

(11)

Consider now k such that M = N n - k. Fix an

arbitrary

sing’

Write and A’ = B’

nf-k-N(A). By

is contained

in a disc of radius 2

Co ð2’

so

by (7)

B’ is contained in a disc B

(y, ðl/2)

for a

point y E B’. By (6)

and

by

the definition of

ffk

we So

by (5)

We

apply

the bounded distortion property

[cf. ( 1 )]

and obtain with the use

of

(9)

Now for every T

multiply

the both sides of the

respective inequality (8), (10)

or

( 11 ) by ~(T),

then sum up these

inequalities

over all T. We

obtain

(~ (B (z, b2/2))

is swallowed

by C).

Hence ~(03C9 ~ B(z, 03B42/3))=0.

As z ~ 03C9 has been chosen

arbitrarily,

we

obtain 11

=0. D

Remark 3. - Observe that

where

d = deg f,

K denotes the number of critical

points

in and

v j -

1

are their

multiplicities.

Indeed

if 03B42

is chosen small

enough,

then every critical

point

is contained in at most one set from the

fn - k -1 (T)

for every

T E sing’ .

Remark 4. - From

(12)

one

immediately

obtains for every A

c ~

Also a related estimate, better than

(3),

holds

Proof of (15). -

Let for

z E cl (Crit+),

see the notation

from the

proof

of Lemma 6. We assumed there but the discussion there holds for every z. If

z ~ B (m, E),

then for every n we have

only decomposition

J =

Jreg ~ Jsing,

where

T ~ Jreg

or

Jsing depending

as

Denote dist and suppose

@&#x3E;0.

We want to estimate

tortion property we have for the branch B -~ T

(12)

Suppose

that sing and fix We have

By

the bounded distortion property I x

III ~

C. To estimate II write

Crit + ) and

denote

by

D the

reciprocal

to the

degree of fM

We have

Summing

up the

respective inequalities

over all T proves

( 15).

D

Remark 5. - One could

slightly modify

the

proofs

of Lemma 6 and

inequality ( 15)

if one observed that

where

d = deg f (observe

that the

right

hand side constant is

independent

of k and

n).

This estimate follows from the fact that for

sing’ for s &#x3E;_ n -

k,

does not contain any critical

point

and for every

~:M2014A;2014M~~2014A;

at most the number

2 d - 2 &#x3E;_ Card (Crit)

of com- ponents

of f S sing)

contain critical

points.

Thus,

in the

proof

of Lemma 6 for

example,

if instead of

(9)

we used

the weaker

inequality

we would also succeed:

Remark 6. - There

exists ~

&#x3E; 0 such that for every E &#x3E;

0,

This fact is stronger than Lemma 6. It follows from

( 14)

and the similar

fact with 11

replaced by

J.1. The latter is a

general phenomenon. Namely

the

following

holds:

PROPOSITION 2. - Let X be a closed nowhere dense subset

of

such

that

f(X)

= X and

f|x

is

expanding.

Then

for

upper limit

capacity defined

Vol. 53, n° 4-1990.

(13)

of

radius s

covering X,

we have

and there exist

C,

K .&#x3E; ~ such that

for

ever~y ~ &#x3E;

0,

Proof (A hint). -

Consider

covering by

squares rather than disc and observe with the use of Koebe’s distortion theorem that there exists an

integer

M such that for every square K

partitioned

into a

family

Jf of

squares of side where r denotes the side of

K,

at least one element of Jf is

disjoint

with X. Next use this observation to

subsequent

divisions

into squares of

sides 1/Mn.

0

Remark 8. - Metric exactness

obviously implies ergodicity of ~.

So

every weak - * limit of

(vn)

is

equivalent

to }i and

.ergodic.

We conclude

that the whole sequence Vn is

weakly - *

convergent to the

unique

measure 11.

Moreover,

the sequence of the densities

F n =

is

equiconti-

nuous on every compact set K

disjoint

with Crit +. This follows from the theorem of Koebe

[H],

Lemma 17.4. I that there exists a universal con- stant C&#x3E;O such that for the disc

B(z,s) disjoint

with Crit +

(cf

the

begin

of Proof of Th.

3),

for every

branchy"

we have

Indeed this allows to estimate the derivative

along

an

arbitrary

vector v

of

length

1

We conclude that the densities converge to

uniformly

on

every K..

(14)

In fact the above convergence holds even in

analytic functions, namely

the

following

holds:

PROPOSITION 3. - For every disc B

(z, E) disjoint

with Crit + the

functions Fn

=

dfn*( )/d

are real

analytic

and subharmonic.

They

can be extended to

complex analytic functions F,~

on the ball

B (z, E/4) c ~ 2,

the extension

of

the disc B

(z, E/4)

c f~2 =

C , uniformly

bounded.

In consequence is

real-analytic

and subharmonic..

Proof. -

For every we have

where

We work in some charts in which we denote

x = (xl, x2~,

For each

branch f-nv

we

estimate, using

the

above,

where

So we have convergence in the

polydisc

in ~2 of radius

s/3. Summing of (16)

over all branches

gives

a bound

independent

of n on

B (z, ~/4~).

So the

family Fn

is

equicontinuous

on compact sets in

B (z, £/4)

and

the limit functions in the uniform convergence

topology

are

analytic.

Subharmonicity

follows from the fact that every

( ~ f ~ ’~)‘ ( 2~,

as the

composi-

tion of the harmonic function

21og~(/~/ I

with the convex

increasing

function exp, is

subharmonic,

see

Note :

Already

after the

completion

of this paper our attention was

drawn to the fact that some of our assertions are

explicitly

contained in

Lyubich’s

papers other than

[L], namely

in

[11 Entropy properties

of rational

endomorphisms

of the Riemann

sphere, Erg.

and

Dyn. Sys.,

Vol.

3, 1983, pp. 351-385.

[2]

A

study

of the

stability

of

dynamics

of rational

functions,

Teoria

Funkcij, Funkcj.

An.

pril. 42, Kharkov, 1984, pp. 72-90 (in Russian).

[3] Dynamics

of rational maps: the

topological picture, Usp.

Mat.

Nauk. ,

Vol.

41, 4, 1986, pp. 35-95.

Lemma I

overlaps

with

[1] Prop. 3, [2]

Lemma 1. 1 and

[3] Prop.

1.10.

Corollary

2 can be found in

[2]

and

overlaps

with

[3] Prop.

1.11. The concept of the

"easy"

set present

already

in

[L]

is

explicit

in

[3]

section

Vol. 53, n° 4-1990.

(15)

1.19. The part p

(ro-1)

= 0 of our Lemma 4 and Theorem 1

[except (ii’)]

can be found there.

REFERENCES

[D] A. DOUADY, Disques de Siegel et anneaux de Herman, Séminaire Bourbaki, No. 677, février 1987.

[D-H] A. DOUADY and J. HUBBARD, Étude dynamique des polynômes complexes, Publ.

Math. Orsay, (2), Vol. 84, (4), p. 85.

[H] E. HILLE, Analytic Function Theory, Boston-New York-Chicago-Atlanta-Dallas-Palo

Alto-Toronto: Ginn and Company, 1962.

[Her] M. HERMAN, Exemples de fractions rationnelles ayant une orbite dense sur la sphère

de Riemann, Bull. Soc. Math. France, Vol. 112, 1984, pp. 93-142.

[Hö] L. HÖRMANDER, An Introduction to Complex Analysis in Several Variables, D. van

Nostrand Company Inc., Princeton, New Jersey, 1966.

[K-S] K. KRZYZEWSKI and W. SZLENK, On Invariant Measures for Expanding Differentiable

Mappings, Studia Math., Vol. 33, 1969, pp. 83-92.

[L] M. Ju. LYUBICH, On a Typical Behaviour of Trajectories for a Rational Map of Sphere, Dokl. Ak. N. U.S.S.R., Vol. 268.1, 1982, pp. 29-32.

[M] M. MISIUREWICZ, Absolutely Continuous Measures for Certain Maps of an Interval, Publications Mathématiques I.H.E.S., Vol. 53, pp. 17-51.

[R] M. REES, Positive Measure Sets of Ergodic Rational Maps, Ann. Sci. Éc. Norm.

Sup., 4e série, Vol. 19, 1986, pp. 383-407.

[S] W. SZLENK, Absolutely Continuous Invariant Measures for Rational Mappings of

the Sphere S2, Geometric Dynamics (Rio de Janeiro, 1981), pp. 767-783, Lect.

Notes Math., Vol. 1007, Springer, Berlin-New York, 1983.

( Manuscript received May 24, 1990.)

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